Home > Publications database > Measurement of $^{2}$H(d,d)$^{2}$H, $^{2}H(d,p)^{3}$H and $^{2}$H(d,n)$^{3}$He Cross Sections in the Energy Range of the Jülich Cyclotron JULIC |
Book/Report | FZJ-2018-01178 |
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1978
Kernforschungsanlage Jülich, Verlag
Jülich
Please use a persistent id in citations: http://hdl.handle.net/2128/17160
Report No.: Juel-1538
Abstract: The d+d system provides the simplest case to study the interaction between composite particles. Recent theoretical developments made by Sawicki$^{1)}$ andPerne and Sandhas$^{2)}$ towards the exact treatment of the four-body problem seem to be encouraging. At present, however, such calculations cannot explain the data in all the details. In view of this it may be interesting to pick out certain aspects of the problem which are accessible to a more phenomenological approach by comparing experimental data with predictions of simpler models. Such a treatment of the d+d system has been carried out in a previous paper$^{3)}$ where the Modified Simple Impulse Approximation (MSIA) model $^{4)}$ was applied to the $^{2}$H(d,dp)n reaction measured under the kinematical conditions favouring thequasi-free d-p scattering. The model gave good fits to the experimental data over a large range of incident energies. In view of the results obtained for the above $\underline{three-body}$ final state, one could naturally ask whether similar features also show up in the $\underline{two-body}$ final state. In the present work we have investigated the two-body final states of the d+d interaction by measuring the angular distribution of the $^{2}$H(d,d)$^{2}$H, $^{2}H(d,p)^{3}$H and $^{2}$H(d,n)$^{3}$ reactions in the energy range of the Jülich cyclotron (i.e. E$_{d}$ = 50-85 MeV).
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